AVS 61st International Symposium & Exhibition | |
Advanced Surface Engineering | Monday Sessions |
Session SE+PS+TF-MoA |
Session: | Pulsed Plasmas in Surface Engineering |
Presenter: | André Anders, Lawrence Berkeley National Laboratory |
Authors: | A. Anders, Lawrence Berkeley National Laboratory Y. Yang, Lawrence Berkeley National Laboratory J. Liu, Lawrence Berkeley National Laboratory Y. Qiu, Lawrence Berkeley National Laboratory |
Correspondent: | Click to Email |
Research in the last years revealed that the plasma in high power impulse magnetron sputtering (HiPIMS) is rich in structure, featuring self-organized patterns [1], plasma flares [2], and azimuthally asymmetric particle jets [3]. Most prominent are drifting regions of enhanced excitation and ionization, which are called ionization zones but sometimes also labeled spokes in analogy to similar phenomena seen in other E x B devices such as Hall thrusters. Fast imaging of ionization zones in HiPIMS revealed the presence of several distinct ionization zones, for example 3-5 zones in the case of sputtering with a 3-inch magnetron at peak currents of the order 100 A. The zone drift velocity is several 1000 m/s, up to 104 m/s, yet much slower than the E x B drift of electrons, which is of the order of 105 m/s. In contrast, when sputtering continuously (dc) at very low current (less than 1 A), and at low pressure (less than 1 Pa), we find only one ionization zone moving at low velocity in the reverse, i.e. the – E x B direction. Increasing the current and pressure tends to split the zone into two and occasionally three zones. The appearance of each zone depends on current and other factors such as the pressure of the process gas. In this contribution, we explore the transition regime between dc operation at low current and HiPIMS operation with high peak currents. Using fast streak and frame imaging cameras we detect even more structures and structure changes than anticipated. We conclude that the discharge and its particle transport is governed by zone-related instabilities and turbulence.
[1] A. Anders, et al., J. Appl. Phys. 111 (2012) 053304.
[2] P.A. Ni, et al., Appl. Phys. Lett. 101 (2012) 224102.
[3] M. Panjan, et al., Plasma Sources Sci. Technol. 23 (2014) 025007.